US11175485B2

US11175485B2 - Zoom optical system, optical apparatus, imaging apparatus and method for manufacturing the zoom optical system

Info

Publication number: US11175485B2
Application number: US16/345,185
Authority: US
Inventors: Kosuke MACHIDA
Original assignee: Nikon Corp
Current assignee: Nikon Corp
Priority date: 2016-11-21
Filing date: 2016-11-21
Publication date: 2021-11-16
Also published as: US20190361212A1; CN109964161A; CN109964161B; EP3543759A4; WO2018092295A1; EP3543759A1; JPWO2018092295A1

Abstract

A zoom optical system comprises, in order from an object: a front lens group (GFS) having a positive refractive power; an M1 lens group (GM1) having a negative refractive power; an M2 lens group (GM2) having a positive refractive power; an RN lens group (GRN) having a negative refractive power; and a subsequent lens group (GRS). Upon zooming, the distance between the front lens group (GFS) and the M1 lens group (GM1) changes, the distance between the M1 lens group (GM1) and the M2 lens group (GM2) changes, and the distance between the M2 lens group (GM2) and the RN lens group (GRN) changes. Upon focusing from an infinite distant object to a short distant object, the RN lens group (GRN) moves.

Description

TECHNICAL FIELD

The present invention relates to a zoom optical system, an optical apparatus and an imaging apparatus including the same, and a method for manufacturing the zoom optical system.

TECHNICAL BACKGROUND

Conventionally, zoom optical systems suitable for photographic cameras, electronic still cameras, video cameras and the like have been proposed (for example, see Patent literature 1).

PRIOR ARTS LIST Patent Document

Patent literature 1: Japanese Laid-Open Patent Publication No. H4-293007(A)

Unfortunately, according to the conventional zoom optical system, reduction in the weight of a focusing lens group is insufficient.

SUMMARY OF THE INVENTION

A zoom optical system according to the present invention comprises, in order from an object: a front lens group having a positive refractive power; an M1 lens group having a negative refractive power; an M2 lens group having a positive refractive power; an RN lens group having a negative refractive power; and a subsequent lens group, wherein upon zooming, a distance between the front lens group and the M1 lens group changes, a distance between the M1 lens group and the M2 lens group changes, and a distance between the M2 lens group and the RN lens group changes, and upon focusing from an infinite distant object to a short distant object, the RN lens group moves.

An optical apparatus according to the present invention comprises the zoom optical system.

An imaging apparatus according to the present invention comprises: the zoom optical system; and an imaging unit that takes an image formed by the zoom optical system.

A method according to the present invention for manufacturing a zoom optical system comprising, in order from an object, a front lens group having a positive refractive power, an M1 lens group having a negative refractive power, an M2 lens group having a positive refractive power, an RN lens group having a negative refractive power, and a subsequent lens group, comprises achieving an arrangement where upon zooming, a distance between the front lens group and the M1 lens group changes, a distance between the M1 lens group and the M2 lens group changes, and a distance between the M2 lens group and the RN lens group changes, wherein upon focusing from an infinite distant object to a short distant object, the RN lens group moves, the subsequent lens group comprises, in order from the object, a lens having a negative refractive power and a lens having a positive refractive power, and a following conditional expression is satisfied,
0.70<(−fN)/fP<2.00

- where
- fN: a focal length of a lens having a strongest negative refractive power in the subsequent lens group, and
- fP: a focal length of a lens having a strongest positive refractive power in the subsequent lens group.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a lens configuration of a zoom optical system according to a first example of this embodiment;

FIG. 2A is graphs showing various aberrations of the zoom optical system according to the first example upon focusing on infinity in the wide-angle end state, and FIG. 2B is graphs showing meridional lateral aberrations (coma aberrations) when blur correction is applied to a rotational blur by 0.30°;

FIG. 3 is graphs showing various aberrations of the zoom optical system according to the first example upon focusing on infinity in the intermediate focal length state;

FIG. 4A is graphs showing various aberrations of the zoom optical system according to the first example upon focusing on infinity in the telephoto end state, and FIG. 4B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 5A, 5B and 5C are graphs showing various aberrations of the zoom optical system according to the first example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 6 shows a lens configuration of a zoom optical system according to a second example of this embodiment;

FIG. 7A is graphs showing various aberrations of the zoom optical system according to the second example upon focusing on infinity in the wide-angle end state, and FIG. 7B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 8 is graphs showing various aberrations of the zoom optical system according to the second example upon focusing on infinity in the intermediate focal length state;

FIG. 9A is graphs showing various aberrations of the zoom optical system according to the second example upon focusing on infinity in the telephoto end state, and FIG. 9B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 10A, 10B and 10C are graphs showing various aberrations of the zoom optical system according to the second example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 11 shows a lens configuration of a zoom optical system according to a third example of this embodiment;

FIG. 12A is graphs showing various aberrations of the zoom optical system according to the third example upon focusing on infinity in the wide-angle end state, and FIG. 12B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 13 is graphs showing various aberrations of the zoom optical system according to the third example upon focusing on infinity in the intermediate focal length state;

FIG. 14A is graphs showing various aberrations of the zoom optical system according to the third example upon focusing on infinity in the telephoto end state, and FIG. 14B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 15A, 15B and 15C are graphs showing various aberrations of the zoom optical system according to the third example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 16 shows a lens configuration of a zoom optical system according to a fourth example of this embodiment;

FIG. 17A is graphs showing various aberrations of the zoom optical system according to the fourth example upon focusing on infinity in the wide-angle end state, and FIG. 17B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 18 is graphs showing various aberrations of the zoom optical system according to the fourth example upon focusing on infinity in the intermediate focal length state;

FIG. 19A is graphs showing various aberrations of the zoom optical system according to the fourth example upon focusing on infinity in the telephoto end state, and FIG. 19B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 20A, 20B and 20C are graphs showing various aberrations of the zoom optical system according to the fourth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 21 shows a lens configuration of a zoom optical system according to a fifth example of this embodiment;

FIG. 22A is graphs showing various aberrations of the zoom optical system according to the fifth example upon focusing on infinity in the wide-angle end state, and FIG. 22B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 23 is graphs showing various aberrations of the zoom optical system according to the fifth example upon focusing on infinity in the intermediate focal length state;

FIG. 24A is graphs showing various aberrations of the zoom optical system according to the fifth example upon focusing on infinity in the telephoto end state, and FIG. 24B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 25A, 25B and 25C are graphs showing various aberrations of the zoom optical system according to the fifth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 26 shows a lens configuration of a zoom optical system according to a sixth example of this embodiment;

FIG. 27A is graphs showing various aberrations of the zoom optical system according to the sixth example upon focusing on infinity in the wide-angle end state, and FIG. 27B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 28 is graphs showing various aberrations of the zoom optical system according to the sixth example upon focusing on infinity in the intermediate focal length state;

FIG. 29A is graphs showing various aberrations of the zoom optical system according to the sixth example upon focusing on infinity in the telephoto end state, and FIG. 29B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 30A, 30B and 30C are graphs showing various aberrations of the zoom optical system according to the sixth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 31 shows a lens configuration of a zoom optical system according to a seventh example of this embodiment;

FIG. 32A is graphs showing various aberrations of the zoom optical system according to the seventh example upon focusing on infinity in the wide-angle end state, and FIG. 32B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 33 is graphs showing various aberrations of the zoom optical system according to the seventh example upon focusing on infinity in the intermediate focal length state;

FIG. 34A is graphs showing various aberrations of the zoom optical system according to the seventh example upon focusing on infinity in the telephoto end state, and FIG. 34B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 35A, 35B and 35C are graphs showing various aberrations of the zoom optical system according to the seventh example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 36 shows a lens configuration of a zoom optical system according to an eighth example of this embodiment;

FIG. 37A is graphs showing various aberrations of the zoom optical system according to the eighth example upon focusing on infinity in the wide-angle end state, and FIG. 37B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 38 is graphs showing various aberrations of the zoom optical system according to the eighth example upon focusing on infinity in the intermediate focal length state;

FIG. 39A is graphs showing various aberrations of the zoom optical system according to the eighth example upon focusing on infinity in the telephoto end state, and FIG. 39B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 40A, 40B and 40C are graphs showing various aberrations of the zoom optical system according to the eighth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 41 shows a lens configuration of a zoom optical system according to a ninth example of this embodiment;

FIG. 42A is graphs showing various aberrations of the zoom optical system according to the ninth example upon focusing on infinity in the wide-angle end state, and FIG. 42B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 43 is graphs showing various aberrations of the zoom optical system according to the ninth example upon focusing on infinity in the intermediate focal length state;

FIG. 44A is graphs showing various aberrations of the zoom optical system according to the ninth example upon focusing on infinity in the telephoto end state, and FIG. 44B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 45A, 45B and 45C are graphs showing various aberrations of the zoom optical system according to the ninth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 46 shows a lens configuration of a zoom optical system according to a tenth example of this embodiment;

FIG. 47A is graphs showing various aberrations of the zoom optical system according to the tenth example upon focusing on infinity in the wide-angle end state, and FIG. 47B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°;

FIG. 48 is graphs showing various aberrations of the zoom optical system according to the tenth example upon focusing on infinity in the intermediate focal length state;

FIG. 49A is graphs showing various aberrations of the zoom optical system according to the tenth example upon focusing on infinity in the telephoto end state, and FIG. 49B is graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°;

FIGS. 50A, 50B and 50C are graphs showing various aberrations of the zoom optical system according to the tenth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 51 shows a lens configuration of a zoom optical system according to an eleventh example of this embodiment;

FIGS. 52A, 52B and 52C are graphs showing various aberrations of the zoom optical system according to the eleventh example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIGS. 53A, 53B and 53C are graphs showing various aberrations of the zoom optical system according to the eleventh example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 54 shows a lens configuration of a zoom optical system according to a twelfth example of this embodiment;

FIGS. 55A, 55B and 55C are graphs showing various aberrations of the zoom optical system according to the twelfth example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIGS. 56A, 56B and 56C are graphs showing various aberrations of the zoom optical system according to the twelfth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 57 shows a lens configuration of a zoom optical system according to a thirteenth example of this embodiment;

FIGS. 58A, 58B and 58C are graphs showing various aberrations of the zoom optical system according to the thirteenth example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIGS. 59A, 59B and 59C are graphs showing various aberrations of the zoom optical system according to the thirteenth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively;

FIG. 60 shows a configuration of a camera including the zoom optical system according to this embodiment; and

FIG. 61 is a flowchart showing a method for manufacturing the zoom optical system according to this embodiment.

DESCRIPTION OF THE EMBODIMENTS

Hereinafter, a zoom optical system, an optical apparatus, and an imaging apparatus of this embodiment are described with reference to the drawings. As shown in FIG. 1, a zoom optical system ZL(1) as an example of a zoom optical system (zoom lens) ZL according to this embodiment comprises, in order from an object: a front lens group GFS having a positive refractive power; an M1 lens group GM1 having a negative refractive power; an M2 lens group GM2 having a positive refractive power; an RN lens group GRN having a negative refractive power; and a subsequent lens group GRS, wherein upon zooming, a distance between the front lens group GFS and the M1 lens group GM1 changes, a distance between the M1 lens group GM1 and the M2 lens group GM2 changes, and a distance between the M2 lens group GM2 and the RN lens group GRN changes, and upon focusing from an infinite distant object to a short distant object, the RN lens group GRN moves.

The zoom optical system ZL according to this embodiment may be a zoom optical system ZL(2) shown in FIG. 6, a zoom optical system ZL(3) shown in FIG. 11, a zoom optical system ZL(4) shown in FIG. 16, a zoom optical system ZL(5) shown in FIG. 21, a zoom optical system ZL(6) shown in FIG. 26, a zoom optical system ZL(7) shown in FIG. 31, a zoom optical system ZL(8) shown in FIG. 36, a zoom optical system ZL(9) shown in FIG. 41, a zoom optical system ZL(10) shown in FIG. 46, a zoom optical system ZL(11) shown in FIG. 51, a zoom optical system ZL(12) shown in FIG. 54, or a zoom optical system ZL(13) shown in FIG. 57.

The zoom optical system of this embodiment includes at least five lens groups, and changes the distances between lens groups upon zooming from the wide-angle end state to the telephoto end state, thereby allowing favorable aberration correction upon zooming to be facilitated. Focusing with the RN lens group GRN can reduce the size and weight of the lens group for zooming. The optical apparatus, the imaging apparatus, and the method for manufacturing the zoom optical system according to this embodiment can also achieve analogous advantageous effects.

In this embodiment, the subsequent lens group GRS may comprise, in order from the object: a lens having a negative refractive power; and a lens having a positive refractive power. Accordingly, various aberrations including the coma aberration can be effectively corrected.

Furthermore, preferably, in the zoom optical system, a following conditional expression (1) is satisfied,
0.70<(−fN)/fP<2.00 (1)

- where
- fN: a focal length of a lens having a strongest negative refractive power in the subsequent lens group GRS, and
- fP: a focal length of a lens having a strongest positive refractive power in the subsequent lens group GRS.

The conditional expression (1) described above defines the ratio of the focal length of the lens that is nearer to the image in the subsequent lens group GRS and has the strongest negative refractive power to the focal length of the lens that is nearer to the image in the subsequent lens group GRS and has the strongest positive refractive power. By satisfying the conditional expression (1), various aberrations including the coma aberration can be effectively corrected.

If the corresponding value of the conditional expression (1) exceeds the upper limit value, the refractive power of the lens that is nearer to the image in the focusing lens group and has a positive refractive power becomes strong, and the coma aberration occurs excessively. Setting of the upper limit value of the conditional expression (1) to 1.90 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (1) be 1.80.

If the corresponding value of the conditional expression (1) falls below the lower limit value, the refractive power of the lens that is nearer to the image in the focusing lens group and has a negative refractive power becomes strong, and the coma aberration is excessively corrected. Setting of the lower limit value of the conditional expression (1) to 0.80 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the lower limit value of the conditional expression (1) be 0.90.

In this embodiment, preferably, upon zooming from a wide-angle end state to a telephoto end state, the front lens group GFS moves toward the object. Accordingly, the entire length of the lens at the wide-angle end state can be reduced, which facilitates reduction in the size of the zoom optical system.

In this embodiment, preferably, the RN lens group GRN comprises: at least one lens having a positive refractive power; and at least one lens having a negative refractive power.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (2),
0.15<(−fTM1)/f1<0.35 (2)

- where
- fTM1: a focal length of the M1 lens group GM1 in a telephoto end state, and
- f1: a focal length of the front lens group GFS.

The conditional expression (2) defines the ratio of the focal length of the M1 lens group GM1 to the focal length of the front lens group GFS in the telephoto end state. By satisfying the conditional expression (2), various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end can be suppressed.

If the corresponding value of the conditional expression (2) exceeds the upper limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (2) to 0.33 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (2) be 0.31.

If the corresponding value of the conditional expression (2) falls below the lower limit value, the refractive power of the M1 lens group GM1 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the lower limit value of the conditional expression (2) to 0.16 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the lower limit value of the conditional expression (2) be 0.17.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (3),
0.20<fTM2/f1<0.40 (3)

- where
- fTM2: a focal length of the M2 lens group GM2 in a telephoto end state, and
- f1: a focal length of the front lens group GFS.

The conditional expression (3) defines the ratio of the focal length of the M2 lens group GM2 to the focal length of the front lens group GFS in the telephoto end state. By satisfying the conditional expression (3), various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end can be suppressed.

If the corresponding value of the conditional expression (3) exceeds the upper limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (3) to 0.37 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (3) be 0.34.

If the corresponding value of the conditional expression (3) falls below the lower limit value, the refractive power of the M2 lens group GM2 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the lower limit value of the conditional expression (3) to 0.22 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the lower limit value of the conditional expression (3) be 0.24.

In this embodiment, preferably, the system further comprises a negative meniscus lens that has a concave surface facing the object, and is adjacent to an image side of the RN lens group GRN. Accordingly, various aberrations including the coma aberration can be effectively corrected.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (4),
1.80<f1/fw<3.50 (4)

- where
- f1: a focal length of the front lens group GFS, and
- fw: a focal length of the zoom optical system in a wide-angle end state.

The conditional expression (4) defines the ratio of the focal length of the front lens group GFS to the focal length of the zoom optical system in the wide-angle end state. By satisfying the conditional expression (4), the size of the lens barrel can be prevented from increasing, and various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end can be suppressed.

If the corresponding value of the conditional expression (4) exceeds the upper limit value, the refractive power of the front lens group GFS becomes weak, and the size of lens barrel increases. Setting of the upper limit value of the conditional expression (4) to 3.30 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (4) to 3.10.

If the corresponding value of the conditional expression (4) falls below the lower limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the lower limit value of the conditional expression (4) to 1.90 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (4) to 2.00, and it is more preferable to set the lower limit value of the conditional expression (4) to 2.10.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (5),
3.70<f1/(−fTM1)<5.00 (5)

- where
- f1: a focal length of the front lens group GFS, and
- fTM1: a focal length of the M1 lens group GM1 in a telephoto end state.

The conditional expression (5) defines the ratio of the focal length of the front lens group GFS to the focal length of the M1 lens group GM1. By satisfying the conditional expression (5), various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end can be suppressed.

If the corresponding value of the conditional expression (5) exceeds the upper limit value, the refractive power of the M1 lens group GM1 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (5) to 4.90 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (5) to 4.80.

If the corresponding value of the conditional expression (5) falls below the lower limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the lower limit value of the conditional expression (5) to 3.90 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (5) to 3.95.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (6),
3.20<f1/fTM2<5.00 (6)

- where
- f1: a focal length of the front lens group GFS, and
- fTM2: a focal length of the M2 lens group GM2 in a telephoto end state.

The conditional expression (6) defines the ratio of the focal length of the front lens group GFS to the focal length of the M2 lens group GM2. By satisfying the conditional expression (6), various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end can be suppressed.

If the corresponding value of the conditional expression (6) exceeds the upper limit value, the refractive power of the M2 lens group GM2 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (6) to 4.80 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (6) to 4.60.

If the corresponding value of the conditional expression (6) falls below the lower limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the lower limit value of the conditional expression (6) to 3.40 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (6) to 3.60.

In this embodiment, preferably, upon zooming, a lens group nearest to the object in the M1 lens group GM1 is fixed with respect to an image surface. Accordingly, degradation in performance due to manufacturing errors is suppressed, which can secure mass-productivity.

In this embodiment, preferably, the M2 lens group GM2 comprises a vibration-proof lens group movable in a direction orthogonal to an optical axis to correct an imaging position displacement due to a camera shake or the like. Such arrangement of the vibration-proof lens group in the M2 lens group GM2 can effectively suppress degradation in performance upon blur correction.

In this embodiment, preferably, the vibration-proof lens group consists of, in order from the object: a lens having a negative refractive power; and a lens having a positive refractive power. Accordingly, degradation in performance upon blur correction can be effectively suppressed.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (7),
1.00<nvrN/nvrP<1.25 (7)

- where
- nvrN: a refractive index of the lens having the negative refractive power in the vibration-proof lens group, and
- nvrP: a refractive index of the lens having the positive refractive power in the vibration-proof lens group.

The conditional expression (7) defines the ratio of the refractive index of the lens that is in the vibration-proof lens group provided in the M2 lens group GM2 and has a negative refractive power to the refractive index of the lens that is in the vibration-proof lens group and has a positive refractive power. By satisfying the conditional expression (7), degradation in performance upon blur correction can be effectively suppressed.

If the corresponding value of the conditional expression (7) exceeds the upper limit value, the refractive index of the lens that is in the vibration-proof lens group and has a positive refractive power decreases, the decentering coma aberration caused upon blur correction excessively occurs, and it becomes difficult to correct the aberration. Setting of the upper limit value of the conditional expression (7) to 1.22 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (7) be 1.20.

If the corresponding value of the conditional expression (7) is in this range, the refractive index of the lens that is in the vibration-proof lens group and has a negative refractive power is appropriate, and the decentering coma aberration upon blur correction is favorably corrected, which is preferable. Setting of the lower limit value of the conditional expression (7) to 1.03 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the lower limit value of the conditional expression (7) be 1.05.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (8),
0.30<νvrN/νvrP<0.90 (8)

- where
- νvrN: an Abbe number of the lens having the negative refractive power in the vibration-proof lens group, and
- νvrP: an Abbe number of the lens having the positive refractive power in the vibration-proof lens group.

The conditional expression (8) defines the ratio of the Abbe number of the lens that is in the vibration-proof lens group and has a negative refractive power to the Abbe number of the lens that is in the vibration-proof lens group and has a positive refractive power. By satisfying the conditional expression (8), degradation in performance upon blur correction can be effectively suppressed.

If the corresponding value of the conditional expression (8) is in this range, the Abbe number of the lens that is in the vibration-proof lens group and has a positive refractive power is appropriate, and the chromatic aberration caused upon blur correction is favorably corrected, which is preferable. Setting of the upper limit value of the conditional expression (8) to 0.85 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (8) be 0.80.

If the corresponding value of the conditional expression (8) falls below the lower limit value, the Abbe number of the lens that is in the vibration-proof lens group and has a negative refractive power decreases, and it becomes difficult to correct the chromatic aberration caused upon blur correction. Setting of the lower limit value of the conditional expression (8) to 0.35 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the lower limit value of the conditional expression (8) be 0.40.

In this embodiment, preferably, the M1 lens group GM1 also comprises a vibration-proof lens group movable in a direction orthogonal to an optical axis to correct an imaging position displacement due to a camera shake or the like. In this case, preferably, the vibration-proof lens group consists of, in order from the object: a lens having a negative refractive power; and a lens having a positive refractive power.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (9),
0.80<nvrN/nvrP<1.00 (9)

The conditional expression (9) defines the ratio of the refractive index of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a negative refractive power to the refractive index of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a positive refractive power. By satisfying the conditional expression (9), degradation in performance upon blur correction can be effectively suppressed.

If the corresponding value of the conditional expression (9) exceeds the upper limit value, the refractive index of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a positive refractive power decreases, and it becomes difficult to correct the decentering coma aberration caused upon blur correction. Setting of the upper limit value of the conditional expression (9) to 0.98 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (9) to 0.96.

If the corresponding value of the conditional expression (9) falls below the lower limit value, the refractive index of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a negative refractive power decreases, and it becomes difficult to correct the decentering coma aberration caused upon blur correction. Setting of the lower limit value of the conditional expression (9) to 0.82 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (9) to 0.84.

In this embodiment, preferably, the zoom optical system satisfies a following conditional expression (10),
1.20<νvrN/νvrP<2.40 (10)

The conditional expression (10) defines the ratio of the Abbe number of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a negative refractive power to the Abbe number of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a positive refractive power. By satisfying the conditional expression (10), degradation in performance upon blur correction can be effectively suppressed.

If the corresponding value of the conditional expression (10) exceeds the upper limit value, the Abbe number of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a positive refractive power significantly decreases. Accordingly, it becomes difficult to correct the chromatic aberration caused upon blur correction. Setting of the upper limit value of the conditional expression (10) to 2.30 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (10) to 2.20.

If the corresponding value of the conditional expression (10) falls below the lower limit value, the Abbe number of the lens that is in the vibration-proof lens group provided in the M1 lens group GM1 and has a negative refractive power significantly decreases. Accordingly, it becomes difficult to correct the chromatic aberration caused upon blur correction. Setting of the lower limit value of the conditional expression (10) to 1.30 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (10) to 1.40.

In this embodiment, preferably, the subsequent lens group GRS comprises a lens having a positive refractive power. Accordingly, various aberrations including the coma aberration can be effectively corrected.

In this case, preferably, the zoom optical system satisfies a following conditional expression (2),
0.15<(−fTM1)/f1<0.35 (2)

Note that the conditional expression (2) is the same as described above. The details are as described above.

Also in this case, if the corresponding value of the conditional expression (2) exceeds the upper limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (2) to 0.33 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (2) be 0.31.

In the case described above, preferably, the zoom optical system satisfies a following conditional expression (3),
0.20<fTM2/f1<0.40 (3)

The conditional expression (3) is the same as described above. The details are as described above.

Also in this case, if the corresponding value of the conditional expression (3) exceeds the upper limit value, the refractive power of the front lens group GFS becomes strong, and it is difficult to correct various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (3) to 0.37 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable that the upper limit value of the conditional expression (3) be 0.34.

In the case described above, preferably, the zoom optical system satisfies a following conditional expression (4),
1.80<f1/fw<3.50 (4)

The conditional expression (4) is the same as described above. The details are as described above.

Also in this case, if the corresponding value of the conditional expression (4) exceeds the upper limit value, the refractive power of the front lens group GFS becomes weak, and the size of lens barrel increases. Setting of the upper limit value of the conditional expression (4) to 3.30 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (4) to 3.10.

Furthermore, in the case described above, preferably, the zoom optical system satisfies a following conditional expression (5),
3.70<f1/(−fTM1)<5.00 (5)

The conditional expression (5) is the same as described above. The details are as described above.

Also in this case, if the corresponding value of the conditional expression (5) exceeds the upper limit value, the refractive power of the M1 lens group GM1 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (5) to 4.90 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (5) to 4.80.

Furthermore, in the case described above, preferably, the zoom optical system satisfies a following conditional expression (6),
3.20<f1/fTM2<5.00 (6)

The conditional expression (6) is the same as described above. The details are as described above.

Also in this case, if the corresponding value of the conditional expression (6) exceeds the upper limit value, the refractive power of the M2 lens group GM2 becomes strong, and it is difficult to suppress variation in various aberrations including the spherical aberration upon zooming from the wide-angle end to the telephoto end. Setting of the upper limit value of the conditional expression (6) to 4.80 can more securely achieve the advantageous effects of this embodiment. To further secure the advantageous effects of this embodiment, it is preferable to set the upper limit value of the conditional expression (6) to 4.60.

An optical apparatus and an imaging apparatus according to this embodiment comprise the zoom optical system having the configuration described above. As a specific example, a camera (corresponding to the imaging apparatus of the invention of the present application) including the aforementioned zoom optical system ZL is described with reference to FIG. 60. As shown in FIG. 60, this camera 1 has a lens assembly configuration including a replaceable imaging lens 2. The zoom optical system having the configuration described above is provided in the imaging lens 2. That is, the imaging lens 2 corresponds to the optical apparatus of the invention of the present application. The camera 1 is a digital camera. Light from an object (subject), not shown, is collected by the imaging lens 2, and reaches an imaging element 3. Accordingly, the light from the subject is imaged by the imaging element 3, and recorded as a subject image in a memory, not shown. As described above, a photographer can take an image of the subject through the camera 1. Note that this camera may be a mirrorless camera, or a single-lens reflex type camera including a quick return mirror.

According to the configuration described above, the camera 1 mounted with the zoom optical system ZL described above in the imaging lens 2 can achieve high-speed AF and silence during AF without increasing the size of the lens barrel by reducing the size and weight of the focusing lens group. Furthermore, variation of aberrations upon zooming from the wide-angle end state to the telephoto end state, and variation of aberrations upon focusing from an infinite distant object to a short distant object can be favorably suppressed, and a favorable optical performance can be achieved.

Subsequently, referring to FIG. 61, an overview of a method for manufacturing the aforementioned zoom optical system ZL is described. First, arrange, in order from an object, a front lens group GFS having a positive refractive power, an M1 lens group GM1 having a negative refractive power, an M2 lens group GM2 having a positive refractive power, an RN lens group GRN having a negative refractive power, and a subsequent lens group GRS (step ST1). Then, achieve a configuration such that upon zooming, a distance between the front lens group GFS and the M1 lens group GM1 changes, a distance between the M1 lens group GM1 and the M2 lens group GM2 changes, and a distance between the M2 lens group GM2 and the RN lens group GRN changes, (step ST2). In this case, achieve a configuration such that upon focusing from an infinite distant object to a short distant object, the RN lens group GRN moves (step ST3), and configure the subsequent lens group GRS to include, in order from the object, a lens having a negative refractive power, and a lens having a positive refractive power (step ST4). Furthermore, arrange each lens so as to satisfy a predetermined conditional expression (step ST5).

EXAMPLES

Hereinafter, zoom optical systems (zoom lens) ZL according to the examples of this embodiment are described with reference to the drawings. FIGS. 1, 6, 11, 16, 21, 26, 31, 36, 41, 46, 51, 54 and 57 are sectional views showing the configurations and refractive power distributions of the zoom optical systems ZL {ZL(1) to ZL(13)} according to first to thirteenth examples. At lower parts of the sectional views of the zoom optical systems ZL(1) to ZL(13), the movement direction of each lens group along the optical axis during zooming from the wide-angle end state (W) to the telephoto end state (T) is indicated by a corresponding arrow. Furthermore, the movement direction during focusing the focusing group GRN from infinity to a short distant object is indicated by an arrow accompanied by characters “FOCUSING.”

FIGS. 1, 6, 11, 16, 21, 26, 31, 36, 41, 46, 51, 54 and 57 show each lens group by a combination of a symbol G and a numeral or alphabet(s), and show each lens by a combination of a symbol L and a numeral. In this case, to prevent the types and numbers of symbols and numerals from increasing and being complicated, the lens groups and the like are indicated using the combinations of symbols and numerals independently on an example-by-example basis. Accordingly, even though the same combinations of symbols and numerals are used among the examples, the combinations do not mean the same configurations.

Tables 1 to 13 are hereinafter shown below. Tables 1 to 13 are tables representing various data in the first to thirteenth examples. In each example, d-line (wavelength 587.562 nm) and g-line (wavelength 435.835 nm) are selected as calculation targets of aberration characteristics.

In [Lens data] tables, the surface number denotes the order of optical surfaces from the object along a light beam traveling direction, R denotes the radius of curvature (a surface whose center of curvature is nearer to the image is assumed to have a positive value) of each optical surface, D denotes the surface distance, which is the distance on the optical axis from each optical surface to the next optical surface (or the image surface), nd denotes the refractive index of the material of an optical element for the d-line, and νd denotes the Abbe number of the material of an optical element with reference to the d-line. The object surface denotes the surface of an object. “∞” of the radius of curvature indicates a flat surface or an aperture. (Stop S) indicates an aperture stop S. The image surface indicates an image surface I. The description of the air refractive index nd=1.00000 is omitted.

In [Various data] tables, f denotes the focal length of the entire zoom lens, FNO denotes the f-number, 2ω denotes the angle of view (represented in units of ° (degree); ω denotes the half angle of view), and Ymax denotes the maximum image height. TL denotes the distance obtained by adding BF to the distance on the optical axis from the lens forefront surface to the lens last surface upon focusing on infinity. BF denotes the distance (back focus) on the optical axis from the lens last surface to the image surface I upon focusing on infinity. Note that these values are represented for zooming states of the wide-angle end (W), the intermediate focal length (M), and the telephoto end (T).

[Variable distance data] tables show the surface distances at surface numbers (e.g.,

surface numbers

5, 13, 25 and 29 in First Example) to which the surface distance of “Variable” in the table representing [Lens data] correspond. This shows the surface distances in the zooming states of the wide-angle end (W), the intermediate focal length (M) and the telephoto end (T) upon focusing on infinity and a short distant object.

[Lens group data] tables show the starting surfaces (the surfaces nearest to the object) and the focal lengths of the first to fifth lens groups (or the sixth lens group).

[Conditional expression corresponding value] tables show values corresponding to the conditional expressions (1) to (10) described above. Here, not all the examples necessarily correspond to all the conditional expressions. Accordingly, the values of the corresponding conditional expressions in each example are shown.

Hereinafter, for all the data values, the listed focal length f, radius of curvature R, surface distance D, other lengths and the like are typically represented in “mm” if not otherwise specified. However, the optical system can exert equivalent optical performances even if being proportionally magnified or proportionally reduced. Consequently, the representation is not limited thereto.

The above descriptions of the tables are common to all the examples. Hereinafter, redundant description is omitted.

First Example

The first example is described with reference to FIG. 1 and Table 1. FIG. 1 shows a lens configuration of a zoom optical system according to the first example of this embodiment. The zoom optical system ZL(1) according to this example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. The sign (+) or (−) assigned to each lens group symbol indicates the refractive power of the corresponding lens group. This similarly applies to all the following examples.

In relation to the embodiment described above, in this configuration, the first lens group G1 corresponds to the front lens group GFS, the second lens group G2 corresponds to the M1 lens group GM1, the third lens group G3 corresponds to the M2 lens group GM2, the fourth lens group G4 corresponds to the RN lens group GRN, and the fifth lens group G5 corresponds to the subsequent lens group GRS.

The first lens group G1 consists of, in order from the object: a positive convexo-planar lens L11 having a convex surface facing the object; and a positive cemented lens consisting of a negative meniscus lens L12 having a convex surface facing the object, and a positive meniscus lens L13 having a convex surface facing the object.

The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a positive biconvex lens L22; a negative biconcave lens L23; and a negative meniscus lens L24 having a concave surface facing the object.

The third lens group G3 consists of, in order from the object: a positive cemented lens consisting of a negative meniscus lens L31 having a convex surface facing the object, and a positive biconvex lens L32; a positive cemented lens consisting of a positive biconvex lens L33, and a negative biconcave lens L34; an aperture stop S; a negative cemented lens consisting of a negative meniscus lens L35 having a convex surface facing the object, and a positive biconvex lens L36; and a positive biconvex lens L37.

The fourth lens group G4 consists of, in order from the object: a positive meniscus lens L41 having a concave surface facing the object; and a negative biconcave lens L42.

The fifth lens group G5 consists of, in order from the object: a negative meniscus lens L51 having a concave surface facing the object; and a positive biconvex lens L52.

In the optical system according to this example, focusing from a long distant object to a short distant object is performed by moving the fourth lens group G4 in the image surface direction.

The zoom optical system according to this example corrects the imaging position displacement due to a camera shake or the like (vibration proof) by moving the positive cemented lens that consists of the negative meniscus lens L31 having the convex surface facing the object and the positive biconvex lens L32 and is included in the third lens group G3 (M2 lens group GM2), in a direction orthogonal to the optical axis.

To correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction may be moved in a direction orthogonal to the optical axis by (f·tan θ)/K. At the wide-angle end in the first example, the vibration proof coefficient is 1.65, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.23 mm. In the telephoto end state in the first example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 1 lists the values of data on the optical system according to this example. In Table 1, f denotes the focal length, and BF denotes the back focus.

TABLE 1

First Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	109.4870	4.600	1.48749	70.31
2	∞	0.200
3	101.1800	1.800	1.62004	36.40
4	49.8109	7.200	1.49700	81.61
5	385.8166	Variable
6	176.0187	1.700	1.69680	55.52
7	31.3680	5.150
8	32.6087	5.500	1.78472	25.64
9	−129.7634	1.447
10	−415.4105	1.300	1.77250	49.62
11	34.3083	4.300
12	−33.1502	1.200	1.85026	32.35
13	−203.5644	Variable
14	70.9040	1.200	1.80100	34.92
15	30.2785	5.900	1.64000	60.20
16	−70.1396	1.500
17	34.0885	6.000	1.48749	70.31
18	−42.6106	1.300	1.80610	40.97
19	401.2557	2.700
20	∞	14.110			(Stop S)
21	350.0000	1.200	1.83400	37.18
22	30.1592	4.800	1.51680	63.88
23	−94.9908	0.200
24	66.3243	2.800	1.80100	34.92
25	−132.5118	Variable
26	−92.0997	2.200	1.80518	25.45
27	−44.0090	6.500
28	−36.9702	1.000	1.77250	49.62
29	68.3346	Variable
30	−24.5000	1.400	1.62004	36.40
31	−41.1519	0.200
32	106.0000	3.800	1.67003	47.14
33	−106.0000	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	100.0	292.0
FNO	4.49	4.86	5.88
2ω	33.96	24.48	8.44
Ymax	21.60	21.60	21.60
TL	190.13	205.07	245.82
BF	39.12	46.45	67.12

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	6.204	21.150	61.895	6.204	21.150	61.895
d13	30.000	22.666	2.000	30.000	22.666	2.000
d25	2.180	3.742	3.895	2.837	4.562	5.614
d29	21.418	19.856	19.703	20.761	19.036	17.984

[Lens group data]

Group	Starting surface	f

G1	1	145.319
G2	6	−29.546
G3	14	38.298
G4	26	−48.034
G5	30	324.470

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.266
(2)	(−fTM1)/f1 = 0.203
(3)	fTM2/f1 = 0.264
(4)	f1/fw = 2.016
(5)	f1/(−fTM1) = 4.918
(6)	f−/fTM2 = 3.794
(7)	nvrN/nvrP = 1.098
(8)	νvrN/νvrP = 0.580

FIGS. 2A and 2B are graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the first example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 3 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the first example upon focusing on infinity in the intermediate focal length state. FIGS. 4A and 4B are graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the first example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 5A, 5B and 5C are graphs showing various aberrations of the zoom optical system according to the first example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

In the aberration graphs of FIGS. 2 to 5, FNO denotes the f-number, NA denotes the numerical aperture, and Y denotes the image height. Note that the spherical aberration graph shows the value of the f-number or the numerical aperture corresponding to the maximum aperture. The astigmatism graph and the distortion graph show the maximum value of the image height. The coma aberration graph shows the value of each image height. d denotes the d-line (λ=587.6 nm), and g denotes the g-line (λ=435.8 nm). In the astigmatism graph, solid lines indicate sagittal image surfaces, and broken lines indicate meridional image surfaces. Note that symbols analogous to those in this example are used also in the aberration graphs in the following examples.

The graphs showing various aberrations show that the zoom optical system according to this example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Second Example

FIG. 6 shows a lens configuration of a zoom optical system according to the second example of the present application. The zoom optical system according to this example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a negative refractive power; a fourth lens group G4 having a positive refractive power; a fifth lens group G5 having a negative refractive power; and a sixth lens group G6 having a positive refractive power.

In relation to the embodiment described above, in this configuration, the first lens group G1 corresponds to the front lens group GFS, the second lens group G2 and the third lens group G3 correspond to the M1 lens group GM1, the fourth lens group G4 corresponds to the M2 lens group GM2, the fifth lens group G5 corresponds to the RN lens group GRN, and the sixth lens group G6 corresponds to the subsequent lens group GRS.

The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a positive biconvex lens L22; and a negative biconcave lens L23.

The third lens group G3 consists of a negative meniscus lens L31 having a concave surface facing the object.

The fourth lens group G4 consists of, in order from the object: a positive cemented lens consisting of a negative meniscus lens L41 having a convex surface facing the object, and a positive biconvex lens L42; a positive cemented lens consisting of a positive biconvex lens L43, and a negative biconcave lens L44; an aperture stop S; a negative cemented lens consisting of a negative meniscus lens L45 having a convex surface facing the object, and a positive biconvex lens L46; and a positive biconvex lens L47.

The fifth lens group G5 consists of, in order from the object: a positive meniscus lens L51 having a concave surface facing the object; and a negative biconcave lens L52.

The sixth lens group G6 consists of, in order from the object: a negative meniscus lens L61 having a concave surface facing the object; and a positive biconvex lens L62.

In the optical system according to this example, focusing from a long distant object to a short distant object is performed by moving the fifth lens group G5 in the image surface direction. The imaging position displacement due to a camera shake or the like is corrected by moving the positive cemented lens that consists of the negative meniscus lens L41 having the convex surface facing the object and the positive biconvex lens L42 and is included in the fourth lens group G4 (M2 lens group GM2), in a direction orthogonal to the optical axis.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. At the wide-angle end in the second example, the vibration proof coefficient is 1.66, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.23 mm. In the telephoto end state in the second example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 2 lists the values of data on the optical system according to this example.

TABLE 2

Second Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	107.5723	4.600	1.48749	70.32
2	∞	0.200
3	96.9007	1.800	1.62004	36.40
4	47.8324	7.200	1.49700	81.61
5	361.3792	Variable
6	139.8663	1.700	1.69680	55.52
7	33.7621	6.806
8	33.5312	5.500	1.78472	25.64
9	−139.8348	0.637
10	−492.0620	1.300	1.80400	46.60
11	35.1115	Variable
12	−34.6163	1.200	1.83400	37.18
13	−377.1306	Variable
14	74.8969	1.200	1.80100	34.92
15	31.6202	5.900	1.64000	60.19
16	−69.0444	1.500
17	34.2668	6.000	1.48749	70.32
18	−42.8334	1.300	1.80610	40.97
19	434.9585	2.700
20	∞	14.312			(Stop S)
21	350.0000	1.200	1.83400	37.18
22	30.4007	4.800	1.51680	63.88
23	−98.0361	0.200
24	68.9306	2.800	1.80100	34.92
25	−129.3404	Variable
26	−90.5065	2.200	1.80518	25.45
27	−44.1796	6.500
28	−37.6907	1.000	1.77250	49.62
29	68.3000	Variable
30	−24.5545	1.400	1.62004	36.40
31	−41.7070	0.200
32	106.0000	3.800	1.67003	47.14
33	−106.0000	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	100.0	292.0
FNO	4.53	4.89	5.88
2ω	33.98	24.48	8.44
Ymax	21.60	21.60	21.60
TL	190.82	206.02	245.82
BF	39.12	46.27	66.46

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.861	18.057	57.861	2.861	18.057	57.861
d11	5.727	5.812	6.883	5.727	5.812	6.883
d13	30.500	23.259	2.000	30.500	23.259	2.000
d25	2.246	3.634	3.634	2.888	4.436	5.329
d29	22.411	21.023	21.023	21.770	20.221	19.329

[Lens group data]

Group	Starting surface	f

G1	1	141.867
G2	6	−104.910
G3	12	−45.774
G4	14	38.681
G5	26	−48.266
G6	30	340.779

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.248
(2)	(−fTM1)/f1 = 0.208
(3)	fTM2/f1 = 0.273
(4)	f1/fw = 1.968
(5)	f1/(−fTM1) = 4.804
(6)	f1/fTM2 = 3.668
(7)	nvrN/nvrP = 1.098
(8)	νvrN/νvrP = 0.580

FIGS. 7A and 7B are graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the second example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 8 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the second example upon focusing on infinity in the intermediate focal length state. FIGS. 9A and 9B are graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the second example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 10A, 10B and 10C are graphs showing various aberrations of the zoom optical system according to the second example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

Third Example

FIG. 11 shows a lens configuration of a zoom optical system according to the third example of the present application. The zoom optical system according to this example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a positive refractive power; a fifth lens group G5 having a negative refractive power; and a sixth lens group G6 having a positive refractive power.

In relation to the embodiment described above, in this configuration, the first lens group G1 corresponds to the front lens group GFS, the second lens group G2 corresponds to the M1 lens group GM1, the third lens group G3 and the fourth lens group G4 correspond to the M2 lens group GM2, the fifth lens group G5 corresponds to the RN lens group GRN, and the sixth lens group G6 corresponds to the subsequent lens group GRS.

The third lens group G3 consists of, in order from the object: a positive cemented lens consisting of a negative meniscus lens L31 having a convex surface facing the object, and a positive biconvex lens L32; a positive cemented lens consisting of a positive biconvex lens L33, and a negative biconcave lens L34; and an aperture stop S.

The fourth lens group G4 consists of, in order from the object: a negative cemented lens consisting of a negative meniscus lens L41 having a convex surface facing the object, and a positive biconvex lens L42; and a positive biconvex lens L43.

In the optical system according to this example, focusing from a long distant object to a short distant object is performed by moving the fifth lens group G5 in the image surface direction. The imaging position displacement due to a camera shake or the like is corrected by moving the positive cemented lens that consists of the negative meniscus lens L31 having the convex surface facing the object and the positive biconvex lens L32 and is included in the third lens group G3 (M2 lens group GM2), in a direction orthogonal to the optical axis.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. At the wide-angle end in the third example, the vibration proof coefficient is 1.65, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.23 mm. In the telephoto end state in the third example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 3 lists the values of data on the optical system according to this example.

TABLE 3

Third Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	106.7563	4.600	1.48749	70.32
2	∞	0.200
3	99.4635	1.800	1.62004	36.40
4	49.2336	7.200	1.49700	81.61
5	332.7367	Variable
6	152.3830	1.700	1.69680	55.52
7	31.0229	5.695
8	32.0867	5.500	1.78472	25.64
9	−139.5695	1.399
10	−403.4713	1.300	1.77250	49.62
11	33.8214	4.300
12	−34.0003	1.200	1.85026	32.35
13	−235.0206	Variable
14	69.3622	1.200	1.80100	34.92
15	29.8420	5.900	1.64000	60.19
16	−71.2277	1.500
17	34.4997	6.000	1.48749	70.32
18	−43.1246	1.300	1.80610	40.97
19	382.2412	2.700
20	∞	Variable			(Stop S)
21	350.0000	1.200	1.83400	37.18
22	30.6178	4.800	1.51680	63.88
23	−88.2508	0.200
24	66.4312	2.800	1.80100	34.92
25	−142.7832	Variable
26	−93.6206	2.200	1.80518	25.45
27	−44.3477	6.500
28	−37.1859	1.000	1.77250	49.62
29	68.3000	Variable
30	−24.9508	1.400	1.62004	36.40
31	−42.7086	0.200
32	106.0000	3.800	1.67003	47.14
33	−106.0000	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	100.0	292.0
FNO	4.49	4.85	5.88
2ω	33.98	24.48	8.44
Ymax	21.60	21.60	21.60
TL	190.26	205.79	245.82
BF	39.12	46.10	67.12

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	5.981	21.510	61.535	5.981	21.510	61.535
d13	30.000	23.014	2.000	30.000	23.014	2.000
d20	14.365	14.107	14.196	14.365	14.107	14.196
d25	2.202	3.476	3.676	2.867	4.301	5.396
d29	21.004	19.988	19.700	20.339	19.163	17.979

[Lens group data]

Group	Starting surface	f

G1	1	145.335
G2	6	−29.607
G3	14	48.974
G4	21	62.364
G5	26	−48.296
G6	30	336.791

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.253
(2)	(−fTM1)/f1 = 0.204
(3)	fTM2/f1 = 0.264
(4)	f1/fw = 2.016
(5)	f1/(−fTM1) = 4.909
(6)	f1/fTM2 = 3.786
(7)	nvrN/nvrP = 1.098
(8)	νvrN/νvrP = 0.580

FIGS. 12A and 12B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the third example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 13 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the third example upon focusing on infinity in the intermediate focal length state. FIGS. 14A and 14B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the third example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 15A, 15B and 15C are graphs showing various aberrations of the zoom optical system according to the third example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

Fourth Example

FIG. 16 shows a lens configuration of a zoom optical system according to the fourth example of the present application. The zoom optical system according to this example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power.

The fifth lens group G5 consists of, in order from the object: a negative meniscus lens L51 having a concave surface facing the object; a positive biconvex lens L52; and a positive meniscus lens L53 having a convex surface facing the object.

In the optical system according to this example, focusing from a long distant object to a short distant object is performed by moving the fourth lens group G4 in the image surface direction. The imaging position displacement due to a camera shake or the like is corrected by moving the positive cemented lens that consists of the negative meniscus lens L31 having the convex surface facing the object and the positive biconvex lens L32 and is included in the third lens group G3 (M2 lens group GM2), in a direction orthogonal to the optical axis.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. At the wide-angle end in the fourth example, the vibration proof coefficient is 1.65, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.23 mm. In the telephoto end state in the fourth example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 4 lists the values of data on the optical system according to this example.

TABLE 4

Fourth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	109.5099	4.600	1.48749	70.32
2	∞	0.200
3	101.8486	1.800	1.62004	36.40
4	49.8873	7.200	1.49700	81.61
5	403.0130	Variable
6	166.1577	1.700	1.69680	55.52
7	31.1882	3.953
8	32.0256	5.500	1.78472	25.64
9	−139.5816	1.553
10	−767.2482	1.300	1.77250	49.62
11	33.9202	4.300
12	−32.8351	1.200	1.85026	32.35
13	−256.2484	Variable
14	69.5902	1.200	1.80100	34.92
15	29.9877	5.900	1.64000	60.19
16	−70.0411	1.500
17	36.2271	6.000	1.48749	70.32
18	−39.9358	1.300	1.80610	40.97
19	820.8027	2.700
20	∞	14.092			(Stop S)
21	427.1813	1.200	1.83400	37.18
22	31.7606	4.800	1.51680	63.88
23	−89.4727	0.200
24	73.5865	2.800	1.80100	34.92
25	−110.0493	Variable
26	−83.7398	2.200	1.80518	25.45
27	−42.9999	6.500
28	−36.8594	1.000	1.77250	49.62
29	73.0622	Variable
30	−26.0662	1.400	1.62004	36.4
31	−40.4068	0.200
32	143.0444	3.035	1.67003	47.14
33	−220.8402	0.200
34	100.4330	2.145	1.79002	47.32
35	170.3325	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	100.0	292.0
FNO	4.48	4.85	5.87
2ω	33.94	24.44	8.42
Ymax	21.60	21.60	21.60
TL	190.21	205.27	245.82
BF	39.12	46.37	67.13

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	5.892	20.953	61.502	5.892	20.953	61.502
d13	30.000	22.752	2.000	30.000	22.752	2.000
d25	2.212	3.707	3.900	2.864	4.521	5.606
d29	21.306	19.811	19.618	20.654	18.997	17.912

[Lens group data]

Group	Starting surface	f

G1	1	145.022
G2	6	−29.562
G3	14	38.233
G4	26	−48.257
G5	30	318.066

[Conditional expression corresponding value]

(1)	(−fN)/fP = 0.947
(2)	(−fTM1)/f1 = 0.204
(3)	fTM2/f1 = 0.264
(4)	f1/fw = 2.011
(5)	f1/(−fTM1) = 4.906
(6)	f1/fTM2 = 3.793
(7)	nvrN/nvrP = 1.098
(8)	νvrN/νvrP = 0.580

FIGS. 17A and 17B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the fourth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 18 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the fourth example upon focusing on infinity in the intermediate focal length state. FIGS. 19A and 19B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the fourth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 20A, 20B and 20C are graphs showing various aberrations of the zoom optical system according to the fourth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

Fifth Example

The fifth example is described with reference to FIGS. 21 to 25 and Table 5. FIG. 21 shows a lens configuration of a zoom optical system according to the fifth example of this embodiment. The zoom optical system ZL(5) according to the fifth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 21.

The first lens group G1 consists of, in order from the object: a positive meniscus lens L11 having a convex surface facing the object; and a positive cemented lens consisting of a negative meniscus lens L12 having a convex surface facing the object, and a positive biconvex lens L13.

The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a positive biconvex lens L22; a negative biconcave lens L23; and a negative cemented lens consisting of a negative biconcave lens L24, and a positive meniscus lens L25 having a convex surface facing the object.

The third lens group G3 consists of, in order from the object: a positive biconvex lens L31; a positive cemented lens consisting of a positive biconvex lens L32 and a negative biconcave lens L33; an aperture stop S; a positive cemented lens consisting of a negative meniscus lens L34 having a convex surface facing the object, and a positive biconvex lens L35; and a positive biconvex lens L36.

The fifth lens group G5 consists of, in order from the object: a negative meniscus lens L51 having a concave surface facing the object; and a positive meniscus lens L52 having a convex surface facing the object. An image surface I is disposed to the image side of the fifth lens group G5.

In the zoom optical system ZL(5) according to the fifth example, the entire fourth lens group G4 constitutes the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the entire fourth lens group G4 in the image surface direction. In the zoom optical system ZL(5) according to the fifth example, the negative cemented lens, which consists of the negative lens L24 and the positive meniscus lens L25 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the fifth example, the vibration proof coefficient is 0.97, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.39 mm. In the telephoto end state in the fifth example, the vibration proof coefficient is 2.01, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.51 mm.

The following Table 5 lists the values of data on the optical system according to the fifth example.

TABLE 5

Fifth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	121.1094	4.980	1.48749	70.31
2	474.6427	0.200
3	104.9110	1.700	1.83400	37.18
4	63.9583	9.069	1.49700	81.73
5	−1816.1542	Variable
6	153.9285	1.000	1.83400	37.18
7	37.0130	9.180
8	41.8122	5.321	1.80518	25.45
9	−148.0087	1.552
10	−153.0936	1.000	1.90366	31.27
11	74.4958	4.888
12	−65.0702	1.000	1.69680	55.52
13	35.9839	3.310	1.83400	37.18
14	121.5659	Variable
15	85.1793	3.534	1.80400	46.60
16	−101.3301	0.200
17	38.9890	5.033	1.49700	81.73
18	−62.2191	1.200	1.95000	29.37
19	378.6744	1.198
20	∞	19.885			(Stop S)
21	44.8832	1.200	1.85026	32.35
22	20.5002	4.485	1.51680	63.88
23	−586.4581	0.200
24	64.4878	2.563	1.62004	36.40
25	−357.2881	Variable
26	−801.6030	2.383	1.80518	25.45
27	−50.3151	1.298
28	−57.1873	1.000	1.77250	49.62
29	26.1668	Variable
30	−21.0000	1.300	1.77250	49.62
31	−28.8136	0.200
32	58.9647	3.137	1.62004	36.40
33	524.5289	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	99.9	292.0
FNO	4.57	4.79	5.88
2ω	33.24	23.82	8.24
Ymax	21.60	21.60	21.60
TL	191.32	204.14	241.16
BF	38.52	42.04	60.52

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	22.163	69.630	2.000	22.163	69.630
d14	41.783	30.929	2.000	41.783	30.929	2.000
d25	2.000	3.259	2.000	2.462	3.867	3.166
d29	14.999	13.740	14.999	14.538	13.133	13.833

[Lens group data]

Group	Starting surface	f

G1	1	167.635
G2	6	39.933
G3	15	37.727
G4	26	−36.765
G5	30	2825.740

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.011
(2)	(−fTM1)/f1 = 0.238
(3)	fTM2/f1 = 0.225
(4)	f1/fw = 2.325
(5)	f1/(−fTM1) = 4.198
(6)	f1/fTM2 = 4.443
(9)	nvrN/nvrP = 0.925
(10)	νvrN/νvrP = 1.493

FIGS. 22A and 22B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the fifth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 23 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the fifth example upon focusing on infinity in the intermediate focal length state. FIGS. 24A and 24B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the fifth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 25A, 25B and 25C are graphs showing various aberrations of the zoom optical system according to the fifth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to fifth example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Sixth Example

The sixth example is described with reference to FIGS. 26 to 30 and Table 6. FIG. 26 shows a lens configuration of a zoom optical system according to the sixth example of this embodiment. The zoom optical system ZL(6) according to the sixth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a negative refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 26.

The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a positive cemented lens consisting of a positive biconvex lens L22 and a negative biconcave lens L23; and a negative cemented lens consisting of a negative biconcave lens L24, and a positive meniscus lens L25 having a convex surface facing the object.

The third lens group G3 consists of, in order from the object: a positive biconvex lens L31; a positive cemented lens consisting of a positive biconvex lens L32 and a negative biconcave lens L33; an aperture stop S; a negative cemented lens consisting of a negative meniscus lens L34 having a convex surface facing the object, and a positive meniscus lens L35 having a convex surface facing the object; and a positive biconvex lens L36.

In the zoom optical system ZL(6) according to the sixth example, the entire fourth lens group G4 constitutes the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the entire fourth lens group G4 in the image surface direction. In the zoom optical system ZL(6) according to the sixth example, the negative cemented lens, which consists of the negative lens L24 and the positive meniscus lens L25 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the sixth example, the vibration proof coefficient is 0.93, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.41 mm. In the telephoto end state in the sixth example, the vibration proof coefficient is 1.90, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.54 mm.

The following Table 6 lists the values of data on the optical system according to the sixth example.

TABLE 6

Sixth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	114.5391	5.639	1.48749	70.31
2	663.8041	0.200
3	103.9783	1.700	1.83400	37.18
4	62.4686	8.805	1.49700	81.73
5	−43979.1830	Variable
6	146.6152	1.000	1.77250	49.62
7	35.8241	11.693
8	37.5245	4.696	1.68893	31.16
9	−254.6834	1.000	1.83400	37.18
10	64.6045	5.066
11	−60.5874	1.000	1.56883	56.00
12	39.1203	2.952	1.75520	27.57
13	93.1442	Variable
14	92.3597	3.688	1.80400	46.60
15	−87.7395	0.200
16	36.8528	5.291	1.49700	81.73
17	−63.3187	1.200	1.95000	29.37
18	264.8384	1.289
19	∞	19.911			(Stop S)
20	52.0583	1.200	1.85026	32.35
21	20.7485	3.983	1.51680	63.88
22	439.3463	0.200
23	64.0215	2.788	1.62004	36.40
24	−130.2911	Variable
25	−343.5287	2.371	1.80518	25.45
26	−47.6881	1.474
27	−51.9782	1.000	1.77250	49.62
28	29.6298	Variable
29	−21.0360	1.300	1.60300	65.44
30	−30.1613	0.200
31	64.8879	2.981	1.57501	41.51
32	614.9077	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	99.9	292.0
FNO	4.59	4.76	5.87
2ω	33.22	23.72	8.22
Ymax	21.60	21.60	21.60
TL	191.32	205.16	240.15
BF	38.52	41.03	60.02

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	23.304	67.717	2.000	23.304	67.717
d13	40.383	30.413	2.000	40.383	30.413	2.000
d24	2.000	3.305	2.001	2.487	3.962	3.248
d28	15.588	14.284	15.587	15.101	13.626	14.340

[Lens group data]

Group	Starting surface	f

G1	1	161.728
G2	6	−38.469
G3	14	38.469
G4	25	−39.083
G5	29	−12107.081

[Conditional expression corresponding value]

(1)	(−fN)/fP = 0.968
(2)	(−fTM1)/f1 = 0.238
(3)	fTM2/f1 = 0.238
(4)	f1/fw = 2.243
(5)	f1/(−fTM1) = 4.204
(6)	f1/fTM2 = 4.204
(9)	nvrN/nvrP = 0.894
(10)	νvrN/νvrP = 2.031

FIGS. 27A and 27B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the sixth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 28 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the sixth example upon focusing on infinity in the intermediate focal length state. FIGS. 29A and 29B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the sixth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 30A, 30B and 30C are graphs showing various aberrations of the zoom optical system according to the sixth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to sixth example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Seventh Example

The seventh example is described with reference to FIGS. 31 to 35 and Table 7. FIG. 31 shows a lens configuration of a zoom optical system according to the seventh example of this embodiment. The zoom optical system ZL(7) according to the seventh example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 31.

The first lens group G1 consists of, in order from the object: a positive biconvex lens L11; and a positive cemented lens consisting of a negative meniscus lens L12 having a convex surface facing the object, and a positive biconvex lens L13.

The third lens group G3 consists of, in order from the object: a positive biconvex lens L31; a positive cemented lens consisting of a positive biconvex lens L32 and a negative biconcave lens L33; an aperture stop S; and a positive cemented lens consisting of a negative meniscus lens L34 having a convex surface facing the object, and a positive biconvex lens L35.

The fifth lens group G5 consists of, in order from the object: a negative meniscus lens L51 having a concave surface facing the object; and a positive biconvex lens L52. An image surface I is disposed to the image side of the fifth lens group G5.

In the zoom optical system ZL(7) according to the seventh example, the entire fourth lens group G4 constitutes the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the entire fourth lens group G4 in the image surface direction. In the zoom optical system ZL(7) according to the seventh example, the negative cemented lens, which consists of the negative lens L24 and the positive meniscus lens L25 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the seventh example, the vibration proof coefficient is 0.96, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.39 mm. In the telephoto end state in the seventh example, the vibration proof coefficient is 2.00, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.51 mm.

The following Table 7 lists the values of data on the optical system according to the seventh example.

TABLE 7

Seventh Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	268.8673	3.827	1.48749	70.31
2	−1922.6559	0.200
3	111.5860	1.700	1.62004	36.40
4	61.6123	8.761	1.49700	81.73
5	−1745.4439	Variable
6	124.2629	1.000	1.77250	49.62
7	34.3759	7.147
8	35.3149	5.189	1.60342	38.03
9	−190.5775	1.000	1.77250	49.62
10	75.4448	4.904
11	−65.2960	1.000	1.67003	47.14
12	37.2634	3.301	1.80518	25.45
13	119.9726	Variable
14	80.9765	3.968	1.77250	49.62
15	−78.4621	0.200
16	33.2120	5.701	1.49700	81.73
17	−56.7466	1.200	1.85026	32.35
18	108.8392	1.685
19	∞	18.569			(Stop S)
20	40.1917	1.200	1.85026	32.35
21	18.3878	4.752	1.54814	45.79
22	−98.0255	Variable
23	−121.4042	2.367	1.75520	27.57
24	−36.6433	2.111
25	−37.5895	1.000	1.77250	49.62
26	35.8631	Variable
27	−21.0000	1.300	1.60311	60.69
28	−30.2149	0.200
29	95.7916	3.938	1.67003	47.14
30	−115.9256	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	99.9	292.0
ENO	4.61	4.79	5.87
2ω	33.52	23.90	8.28
Ymax	21.60	21.60	21.60
TL	191.32	207.98	243.25
BF	38.52	41.37	61.52

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	25.429	72.273	2.000	25.429	72.273
d13	43.342	33.718	2.000	43.342	33.718	2.000
d22	2.000	3.210	3.710	2.512	3.900	5.147
d26	19.235	18.025	17.525	18.723	17.335	16.088

[Lens group data]

Group	Starting surface	f

G1	1	169.647
G2	6	−39.988
G3	14	38.817
G4	23	−37.515
G5	27	207.702

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.529
(2)	(−fTM1)/f1 = 0.236
(3)	fTM2/f1 = 0.229
(4)	f1/fw = 2.353
(5)	f1/(−fTM1) = 4.242
(6)	f1/fTM2 = 4.370
(9)	nvrN/nvrP = 0.925
(10)	νvrN/νvrP = 1.852

FIGS. 32A and 32B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the seventh example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 33 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the seventh example upon focusing on infinity in the intermediate focal length state. FIGS. 34A and 34B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the seventh example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 35A, 35B and 35C are graphs showing various aberrations of the zoom optical system according to the seventh example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to seventh example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Eighth Example

The eighth example is described with reference to FIGS. 36 to 40 and Table 8. FIG. 36 shows a lens configuration of a zoom optical system according to the eighth example of this embodiment. The zoom optical system ZL(8) according to the eighth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 36.

The fifth lens group G5 consists of: a negative meniscus lens L51 having a concave surface facing the object; and a positive biconvex lens L52. An image surface I is disposed to the image side of the fifth lens group G5.

In the zoom optical system ZL(8) according to the eighth example, the positive meniscus lens L41 and the negative lens L42 in the fourth lens group G4 constitute the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the positive meniscus lens L41 and the negative lens L42 in the fourth lens group G4 in the image surface direction. In the zoom optical system ZL(8) according to the eighth example, the negative cemented lens, which consists of the negative lens L24 and the positive meniscus lens L25 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the eighth example, the vibration proof coefficient is 1.05, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.36 mm. In the telephoto end state in the eighth example, the vibration proof coefficient is 2.20, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.46 mm.

The following Table 8 lists the values of data on the optical system according to the eighth example.

TABLE 8

Eighth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	384.8872	4.307	1.48749	70.31
2	−459.3665	0.200
3	108.5471	1.700	1.62004	36.40
4	59.1633	8.722	1.49700	81.73
5	−3828.8091	Variable
6	116.0785	1.000	1.77250	49.62
7	33.3782	6.789
8	34.8547	5.123	1.64769	33.73
9	−166.2311	1.000	1.80400	46.60
10	68.6485	5.021
11	−58.3172	1.000	1.66755	41.87
12	33.1524	3.543	1.80518	25.45
13	108.5224	Variable
14	80.6236	4.111	1.77250	49.62
15	−73.7947	0.200
16	32.8485	5.846	1.49700	81.73
17	−53.4390	1.200	1.85026	32.35
18	100.1735	1.748
19	∞	17.032			(Stop S)
20	45.6071	1.200	1.80100	34.92
21	18.9488	5.048	1.54814	45.79
22	−90.5382	Variable
23	−106.0821	2.387	1.72825	28.38
24	−35.2284	2.066
25	−36.8890	1.000	1.77250	49.62
26	46.9619	Variable
27	−21.5153	1.300	1.60311	60.69
28	−31.7338	0.200
29	126.4587	3.612	1.77250	49.62
30	−132.9868	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	99.9	292.0
FNO	4.60	4.77	5.88
2ω	33.56	23.82	8.26
Ymax	21.60	21.60	21.60
TL	192.32	210.67	244.12
BF	38.52	40.08	57.94

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	25.713	69.580	2.000	25.713	69.580
d13	40.783	32.701	2.000	40.783	32.701	2.000
d22	2.000	3.163	5.584	2.559	3.917	7.234
d26	23.661	23.661	23.661	23.103	22.908	22.012

[Lens group data]

Group	Starting surface	f

G1	1	164.404
G2	6	−37.386
G3	14	38.634
G4	23	−43.744
G5	27	272.771

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.378
(2)	(−fTM1)/f1 = 0.227
(3)	fTM2/f1 = 0.235
(4)	f1/fw = 2.280
(5)	f1/(−fTM1) = 4.397
(6)	f1/fTM2 = 4.255
(9)	nvrN/nvrP = 0.924
(10)	νvrN/νvrP = 1.645

FIGS. 37A and 37B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the eighth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 38 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the eighth example upon focusing on infinity in the intermediate focal length state. FIGS. 39A and 39B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the eighth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 40A, 40B and 40C are graphs showing various aberrations of the zoom optical system according to the eighth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to eighth example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Ninth Example

The ninth example is described with reference to FIGS. 41 to 45 and Table 9. FIG. 41 shows a lens configuration of a zoom optical system according to the ninth example of this embodiment. The zoom optical system ZL(9) according to the ninth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 41.

The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a positive meniscus lens L22 having a convex surface facing the object; and a negative cemented lens consisting of a negative biconcave lens L23, and a positive meniscus lens L24 having a convex surface facing the object.

In the zoom optical system ZL(9) according to the ninth example, the entire fourth lens group G4 constitutes the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the entire fourth lens group G4 in the image surface direction. In the zoom optical system ZL(9) according to the ninth example, the negative cemented lens, which consists of the negative lens L23 and the positive meniscus lens L24 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the ninth example, the vibration proof coefficient is 1.02, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.37 mm. In the telephoto end state in the ninth example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 9 lists the values of data on the optical system according to the ninth example.

TABLE 9

Ninth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	494.4763	3.486	1.48749	70.31
2	−654.7200	0.200
3	104.3848	1.700	1.62004	36.40
4	60.0944	8.673	1.49700	81.73
5	−2277.9468	Variable
6	131.3496	1.300	1.80400	46.60
7	35.6812	7.900
8	36.7192	2.871	1.68893	31.16
9	62.4101	4.726
10	−66.4912	1.000	1.70000	48.11
11	36.3174	3.414	1.80518	25.45
12	127.2974	Variable
13	90.0733	3.862	1.80400	46.60
14	−78.6804	0.200
15	33.8033	5.583	1.49700	81.73
16	−57.6791	1.200	1.85026	32.35
17	101.7237	1.726
18	∞	19.598			(Stop S)
19	49.9975	1.200	1.85026	32.35
20	20.1023	4.713	1.54814	45.79
21	−72.4003	Variable
22	−158.4470	2.458	1.71736	29.57
23	−37.7406	1.732
24	−39.9149	1.000	1.77250	49.62
25	43.7406	Variable
26	−22.3495	1.300	1.69680	55.52
27	−32.8093	0.200
28	139.7659	3.301	1.80610	40.97
29	−141.5832	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	99.9	292.0
FNO	4.68	4.85	5.88
2ω	33.48	23.86	8.26
Ymax	21.60	21.60	21.60
TL	192.32	208.96	243.67
BF	38.32	41.06	60.32

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	26.074	74.834	2.000	26.074	77.834
d12	45.487	35.318	2.000	45.487	35.318	2.000
d21	2.000	3.315	2.845	2.597	4.123	4.511
d25	21.171	19.856	20.326	20.574	19.048	18.660

[Lens group data]

Group	Starting surface	f

G1	1	171.348
G2	6	−41.929
G3	13	40.969
G4	22	−45.959
G5	26	423.598

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.209
(2)	(−fTM1)/f1 = 0.245
(3)	fTM2/f1 = 0.239
(4)	f1/fw = 2.377
(5)	f1/(−fTM1) = 4.087
(6)	f1/fTM2 = 4.182
(9)	nvrN/nvrP = 0.942
(10)	νvrN/νvrP = 1.890

FIGS. 42A and 42B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the ninth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 43 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the ninth example upon focusing on infinity in the intermediate focal length state. FIGS. 44A and 44B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the ninth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 45A, 45B and 45C are graphs showing various aberrations of the zoom optical system according to the ninth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to ninth example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Tenth Example

The tenth example is described with reference to FIGS. 46 to 50 and Table 10. FIG. 46 shows a lens configuration of a zoom optical system according to the tenth example of this embodiment. The zoom optical system ZL(10) according to the tenth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in the directions indicated by the respective arrows in FIG. 46.

The first lens group G1 consists of, in order from the object: a positive cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a positive biconvex lens L12; and a positive meniscus lens L13 having a convex surface facing the object.

The second lens group G2 consists of, in order from the object: a positive biconvex lens L21; a negative biconcave lens L22; a positive meniscus lens L23 having a convex surface facing the object; and a negative cemented lens consisting of a negative biconcave lens L24, and a positive meniscus lens L25 having a convex surface facing the object.

The fourth lens group G4 consists of, in order from the object: a positive biconvex lens L41; and a negative biconcave lens L42.

In the zoom optical system ZL(10) according to the tenth example, the entire fourth lens group G4 constitutes the focusing lens group, and focusing from a long distant object to a short distant object is performed by moving the entire fourth lens group G4 in the image surface direction. In the zoom optical system ZL(10) according to the tenth example, the negative cemented lens, which consists of the negative lens L24 and the positive meniscus lens L25 and is included in the second lens group G2 (M1 lens group GM1), constitutes the vibration-proof lens group movable in a direction perpendicular to the optical axis, and corrects the imaging position displacement (image blur on the image surface I) due to a camera shake or the like.

Note that to correct a rotational blur with an angle θ at a lens having the focal length f of the entire system and a vibration proof coefficient K (the ratio of the amount of image movement on the image forming surface to the amount of movement of the movable lens group upon blur correction), the movable lens group for blur correction is moved in a direction orthogonal to the optical axis by (f·tan θ)/K. In the wide-angle end state in the tenth example, the vibration proof coefficient is 1.01, and the focal length is 72.1 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.30° is 0.37 mm. In the telephoto end state in the tenth example, the vibration proof coefficient is 2.10, and the focal length is 292.0 mm. Accordingly, the amount of movement of the vibration-proof lens group to correct a rotational blur by 0.20° is 0.49 mm.

The following Table 10 lists the values of data on the optical system according to the tenth example.

TABLE 10

Tenth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	139.3408	1.700	1.64769	33.73
2	77.5654	9.455	1.49700	81.73
3	−496.0322	0.200
4	144.5249	3.734	1.48749	70.31
5	357.2933	Variable
6	142.3498	3.303	1.84666	23.80
7	−361.0297	1.824
8	−451.3220	1.300	1.83400	37.18
9	33.3045	7.193
10	35.8308	3.147	1.71736	29.57
11	69.2532	4.718
12	−63.1663	1.000	1.66755	41.87
13	34.7105	3.239	1.80518	25.45
14	102.2323	Variable
15	73.7312	3.697	1.77250	49.62
16	−95.2978	0.200
17	33.5557	5.512	1.49700	81.73
18	−68.5312	1.200	1.90366	31.27
19	129.3820	1.534
20	∞	17.193			(Stop S)
21	40.0826	1.200	1.85026	32.35
22	17.3868	5.268	1.56732	42.58
23	−141.3282	Variable
24	297.2824	2.624	1.64769	33.73
25	−42.2438	0.835
26	−48.9103	1.000	1.77250	49.62
27	31.0082	Variable
28	−22.3095	1.300	1.69680	55.52
29	−31.0148	0.200
30	73.8865	3.135	1.80100	34.92
31	3043.5154	BF
Image surface	∞

[Various data]

Zooming ratio 4.05

	W	M	T

f	72.1	100.0	292.0
FNO	4.65	4.93	5.88
2ω	33.24	23.86	8.28
Ymax	21.60	21.60	21.60
TL	192.32	206.35	244.34
BF	38.32	42.77	60.32

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.000	22.642	74.835	2.000	22.642	74.835
d14	44.818	33.757	2.000	44.818	33.757	2.000
d23	2.000	3.329	2.024	2.604	4.116	3.661
d27	19.472	18.143	19.448	18.869	17.356	17.812

[Lens group data]

Group	Starting surface	f

G1	1	176.000
G2	6	−42.283
G3	15	38.971
G4	24	−44.470
G5	28	381.600

[Conditional expression corresponding value]

(1)	(−fN)/fP = 1.286
(2)	(−fTM1)/f1 = 0.240
(3)	fTM2/f1 = 0.221
(4)	f1/fw = 2.441
(5)	f1/(−fTM1) = 4.162
(6)	f1/fTM2 = 4.516
(9)	nvrN/nvrP = 0.924
(10)	νvrN/νvrP = 1.645

FIGS. 47A and 47B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the tenth example upon focusing on infinity in the wide-angle end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.30°, respectively. FIG. 48 is graphs showing various aberrations of the zoom optical system having the vibration-proof function according to the tenth example upon focusing on infinity in the intermediate focal length state. FIGS. 49A and 49B are graphs showing various aberrations of the zoom optical system having a vibration-proof function according to the tenth example upon focusing on infinity in the telephoto end state, and graphs showing meridional lateral aberrations when blur correction is applied to a rotational blur by 0.20°, respectively. FIGS. 50A, 50B and 50C are graphs showing various aberrations of the zoom optical system according to the tenth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

The graphs showing various aberrations show that the zoom optical system according to tenth example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Eleventh Example

The eleventh example is described with reference to FIGS. 51, 52 and 53 and Table 11. FIG. 51 shows a lens configuration of a zoom optical system according to the eleventh example of this embodiment. The zoom optical system ZL(11) according to the eleventh example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. An aperture stop S is provided in the third lens group G3. An image surface I is provided to face the image surface side of the fifth lens group G5.

The first lens group G1 consists of, in order from the object: a positive biconvex lens L11; and a positive cemented lens consisting of a negative meniscus lens L12 having a convex surface facing the object, and a positive meniscus lens L13 having a convex surface facing the object.

The second lens group G2 consists of, in order from the object: a negative cemented lens consisting of a negative biconcave lens L21, and a positive meniscus lens L22 having a convex surface facing the object; and a negative biconcave lens L23.

The third lens group G3 consists of, in order from the object: a positive biconvex lens L31; an aperture stop S; a positive cemented lens consisting of a positive biconvex lens L32 and a negative biconcave lens L33; a positive cemented lens consisting of a negative meniscus lens L34 having a convex surface facing the object, and a positive biconvex lens L35; and a positive meniscus lens L36 having a convex surface facing the object.

The fourth lens group G4 consists of a negative cemented lens consisting of a positive meniscus lens L41 having a concave surface facing the object, and a negative biconcave lens L42.

The fifth lens group G5 consists of a positive biconvex lens L51.

In the optical system according to the eleventh example, focusing from a long distant object to a short distant object is performed by moving the fourth lens group G4 (RN lens group GRN) in the image surface direction. Preferably, the second lens group G2 (M1 lens group GM1) constitutes the vibration-proof lens group having displacement components in the optical axis and a direction perpendicular to the optical axis, and performs image blur correction (vibration proof, and camera shake correction) on the image surface I.

The following Table 11 lists the values of data on the optical system according to the eleventh example.

TABLE 11

Eleventh Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	91.1552	6.167	1.51680	63.88
2	−844.6033	0.204
3	92.5357	1.500	1.64769	33.73
4	45.6802	6.598	1.48749	70.31
5	154.0927	Variable
6	−211.4795	1.000	1.69680	55.52
7	22.5821	3.677	1.80518	25.45
8	60.3602	2.652
9	−46.9021	1.000	1.77250	49.62
10	299.7358	Variable
11	48.8916	3.796	1.69680	55.52
12	−131.4333	1.000
13	∞	1.000			(Stop S)
14	39.8799	4.932	1.69680	55.52
15	−49.6069	1.000	1.85026	32.35
16	72.3703	8.805
17	57.3477	1.000	1.80100	34.92
18	18.1075	6.038	1.48749	70.31
19	−116.1586	0.200
20	26.5494	3.513	1.62004	36.40
21	96.5593	Variable
22	−119.7021	3.510	1.74950	35.25
23	−16.6839	1.000	1.69680	55.52
24	25.6230	Variable
25	124.9308	2.143	1.48749	70.31
26	−480.8453	BF
Image surface	∞

[Various data]

Zooming ratio 4.12

	W	M	T

f	71.4	100.0	294.0
FNO	4.56	4.26	5.89
2ω	22.82	16.04	5.46
Ymax	14.25	14.25	14.25
TL	159.32	185.24	219.32
BF	45.32	39.43	70.09

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	2.881	37.560	65.654	2.881	37.560	65.654
d10	29.543	26.683	2.000	29.543	26.683	2.000
d21	5.002	5.002	5.002	5.295	5.470	5.772
d24	15.836	15.836	15.836	15.543	15.368	15.066

[Lens group data]

Group	Starting surface	f

G1	1	146.976
G2	6	−31.771
G3	11	30.544
G4	22	−32.594
G5	25	203.039

[Conditional expression corresponding value]

(2)	(−fTM1)/f1 = 0.216
(3)	fTM2/f1 = 0.208
(4)	f1/fw = 2.058
(5)	f1/(−fTM1) = 4.626
(6)	f1/fTM2 = 4.809

FIGS. 52A, 52B and 52C are graphs showing various aberrations of the zoom optical system according to the eleventh example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

FIGS. 53A, 53B and 53C are graphs showing various aberrations of the zoom optical system according to the eleventh example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively.

Twelfth Example

The twelfth example is described with reference to FIGS. 54, 55 and 56 and Table 12. FIG. 54 shows a lens configuration of a zoom optical system according to the twelfth example of this embodiment. The zoom optical system ZL(12) according to the twelfth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power.

The third lens group G3 consists of, in order from the object: a positive biconvex lens L31; a positive cemented lens consisting of a positive biconvex lens L32 and a negative biconcave lens L33; an aperture stop S; a positive cemented lens consisting of a negative meniscus lens L34 having a convex surface facing the object, and a positive biconvex lens L35; and a positive meniscus lens L36 having a convex surface facing the object.

The fifth lens group G5 consists of a positive meniscus lens L51 having a convex surface facing the object.

In the optical system according to the twelfth example, focusing from a long distant object to a short distant object is performed by moving the fourth lens group G4 in the image surface direction. In this example, preferably, the second lens group G2 (M1 lens group GM1) constitutes the vibration-proof lens group having displacement components in the optical axis and a direction perpendicular to the optical axis, and performs image blur correction (vibration proof, and camera shake correction) on the image surface I.

The following Table 12 lists the values of data on the optical system according to the twelfth example.

TABLE 12

Twelfth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	100.0120	5.590	1.51680	63.88
2	−356.7115	0.200
3	87.0822	1.500	1.62004	36.40
4	36.8924	7.184	1.51680	63.88
5	131.1594	Variable
6	−122.1413	1.000	1.69680	55.52
7	20.4910	3.496	1.80518	25.45
8	49.8357	2.470
9	−48.8699	1.000	1.77250	49.62
10	8360.2394	Variable
11	56.6713	3.785	1.58913	61.22
12	−64.2309	0.200
13	35.4309	4.669	1.48749	70.31
14	−48.4394	1.000	1.80100	34.92
15	159.7328	1.860
16	∞	16.684			(Stop S)
17	57.8297	1.000	1.80100	34.92
18	19.6163	4.946	1.48749	70.31
19	−96.4204	0.200
20	27.1066	2.717	1.62004	36.40
21	65.2029	Variable
22	−157.1131	3.395	1.64769	33.73
23	−22.3553	1.000	1.56883	56.00
24	25.0407	Variable
25	46.5745	2.500	1.62004	36.40
26	60.0000
Image surface	∞

[Various data]

Zooming ratio 4.29

	W	M	T

f	68.6	100.0	294.0
ENO	4.69	4.72	6.10
2ω	23.74	16.04	5.46
Ymax	14.25	14.25	14.25
TL	164.32	184.76	221.32
BF	38.52	38.73	64.73

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	4.964	31.058	63.669	4.964	31.058	63.669
d10	29.909	24.050	2.000	29.909	24.050	2.000
d21	3.666	4.368	2.697	4.068	4.962	3.755
d24	20.866	20.163	21.834	20.464	19.569	20.776

[Lens group data]

Group	Starting surface	f

G1	1	137.939
G2	6	−30.083
G3	11	34.644
G4	22	−42.585
G5	25	313.363

[Conditional expression corresponding value]

(2)	(−fTM1)/f1 = 0.218
(3)	fTM2/f1 = 0.251
(4)	f1/fw = 2.011
(5)	f1/(−fTM1) = 4.585
(6)	f1/fTM2 = 3.982

FIGS. 55A, 55B and 55C are graphs showing various aberrations of the zoom optical system according to the twelfth example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. FIGS. 56A, 56B and 56C are graphs showing various aberrations of the zoom optical system according to the twelfth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. The graphs showing various aberrations show that the zoom optical system according to this example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

Thirteenth Example

The thirteenth example is described with reference to FIGS. 57, 58 and 59 and Table 13. FIG. 57 shows a lens configuration of a zoom optical system according to the thirteenth example of this embodiment. The zoom optical system ZL(13) according to the thirteenth example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power.

The fourth lens group G4 consists of: a negative cemented lens consisting of a positive meniscus lens L41 having a concave surface facing the object, and a negative biconcave lens L42; and a negative meniscus lens L43 having a convex surface facing the object.

In the optical system according to the thirteenth example, focusing from a long distant object to a short distant object is performed by moving the fourth lens group G4 in the image surface direction. In this example, preferably, the second lens group G2 (M1 lens group GM1) constitutes the vibration-proof lens group having displacement components in the optical axis and a direction perpendicular to the optical axis, and performs image blur correction (vibration proof, and camera shake correction) on the image surface I.

The following Table 13 lists the values of data on the optical system according to the thirteenth example.

TABLE 13

Thirteenth Example

[Lens data]

Surface No.	R	D	nd	νd

Object surface	∞
1	102.5193	5.542	1.51680	63.88
2	−366.1796	0.200
3	90.4094	1.500	1.62004	36.40
4	37.8518	7.229	1.51680	63.88
5	144.7539	Variable
6	−163.5053	1.000	1.69680	55.52
7	20.5835	3.475	1.80518	25.45
8	48.1602	2.598
9	−47.4086	1.000	1.77250	49.62
10	4634.3570	Variable
11	57.6094	3.843	1.58913	61.22
12	−66.7307	0.200
13	36.4629	4.709	1.48749	70.31
14	−48.7603	1.000	1.80100	34.92
15	206.1449	1.786
16	∞	16.497			(Stop S)
17	55.1101	1.000	1.80100	34.92
18	19.3181	4.785	1.48749	70.31
19	−100.3387	0.200
20	26.0254	2.707	1.62004	36.40
21	57.5286	Variable
22	−201.9970	3.376	1.64769	33.73
23	−22.7237	1.000	1.56883	56.00
24	29.2295	1.172
25	34.9681	1.000	1.79952	42.09
26	26.1166	Variable
27	39.9439	2.135	1.62004	36.40
28	60.0000	BF
Image surface	∞

[Various data]

Zooming ratio 4.28

	W	M	T

f	68.7	100.0	294.0
FNO	4.70	4.73	6.06
2ω	23.74	16.08	5.48
Ymax	14.25	14.25	14.25
TL	164.32	184.47	221.32
BF	38.52	38.72	64.52

[Variable distance data]

				W	M	T
	W	M	T	Short	Short	Short
	Infinity	Infinity	Infinity	distance	distance	distance

d5	4.000	30.052	63.492	4.000	30.052	63.492
d10	30.492	24.393	2.000	30.492	24.393	2.000
d21	3.686	4.454	2.923	4.052	4.994	3.907
d26	19.668	18.899	20.430	19.301	18.359	19.446

[Lens group data]

Group	Starting surface	f

G1	1	138.289
G2	6	−30.436
G3	11	34.256
G4	22	−36.764
G5	27	185.180

[Conditional expression corresponding value]

(2)	(−fTM1)/f1 = 0.220
(3)	fTM2/f1 = 0.248
(4)	f1/fw = 2.013
(5)	f1/(−fTM1) = 4.544
(6)	f1/fTM2 = 4.037

FIGS. 58A, 58B and 58C are graphs showing various aberrations of the zoom optical system according to the thirteenth example upon focusing on infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. FIGS. 59A, 59B and 59C are graphs showing various aberrations of the zoom optical system according to the thirteenth example upon focusing on a short distant object in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. The graphs showing various aberrations show that the zoom optical system according to this example favorably corrects the various aberrations and has excellent image forming performances from the wide-angle end state to the telephoto end state, and further has excellent image forming performances also upon focusing on a short distant object.

According to each of the examples described above, reduction in size and weight of the focusing lens group can achieve high-speed AF and silence during AF without increasing the size of the lens barrel, and the zoom optical system can be achieved that favorably suppresses variation of aberrations upon zooming from the wide-angle end state to the telephoto end state, and variation of aberrations upon focusing from an infinite distant object to a short distant object.

Here, each of the examples described above represents a specific example of the invention of the present application. The invention of the present application is not limited thereto.

Note that the following details can be appropriately adopted in a range without impairing the optical performance of the zoom optical system of the present application.

The five-group configurations and the six-group configurations have been described as the numeric examples of the zoom optical systems of the present application. However, the present application is not limited thereto. Zoom optical systems having other group configurations (for example, seven-group ones and the like) can also be configured. Specifically, a zoom optical system having a configuration where a lens or a lens group is added to the zoom optical system of the present application at a position nearest to the object or to the image surface may be configured. Note that the lens group indicates a portion that has at least one lens and is separated by air distances varying upon zooming.

The lens surfaces of the lenses constituting the zoom optical system of the present application may be spherical surfaces, plane surfaces, or aspherical surfaces. A case where the lens surface is a spherical surface or a plane surface facilitates lens processing and assembly adjustment, and can prevent the optical performance from being reduced owing to the errors in lens processing or assembly adjustment. Consequently, the case is preferable. It is also preferable because reduction in depiction performance is small even when the image surface deviates. In a case where the lens surface is an aspherical surface, the surface may be an aspherical surface made by a grinding process, a glass mold aspherical surface made by forming glass into an aspherical shape with a mold, or a composite type aspherical surface made by forming resin provided on the glass surface into an aspherical shape. The lens surface may be a diffractive surface. The lens may be a gradient index lens (GRIN lens) or a plastic lens.

An antireflection film having a high transmissivity over a wide wavelength range may be applied to the lens surfaces of the lenses constituting the zoom optical system of the present application. This reduces flares and ghosts, and can achieve a high optical performance having a high contrast.

According to the configurations described above, this camera 1 mounted with the zoom optical system according to the first example as the imaging lens 2 can achieve high-speed AF and silence during AF without increasing the size of the lens barrel, by reducing the size and weight of the focusing lens group, can favorably suppresses variation of aberrations upon zooming from the wide-angle end state to the telephoto end state, and variation of aberrations upon focusing from an infinite distant object to a short distant object, and can achieve a favorable optical performance. Note that possible configurations of cameras mounted with the zoom optical systems according to the second to seventh examples described above as the imaging lens 2 can also exert the advantageous effects analogous to those of the camera 1 described above.

EXPLANATION OF NUMERALS AND CHARACTERS


G1	First lens group	G2	Second lens group
G3	Third lens group	G4	Fourth lens group
G5	Fifth lens group	GFS	Front lens group
GM1	M1 lens group	GM2	M2 lens group
GRN	RN lens group	GRS	Subsequent lens group
I	Image surface	S	Aperture stop

Claims

The invention claimed is:

1. A zoom optical system comprising, in order from an object: a front lens group having a positive refractive power; an M1 lens group having a negative refractive power; an M2 lens group having a positive refractive power; an RN lens group having a negative refractive power; and a subsequent lens group, wherein

upon zooming, a distance between the front lens group and the M1 lens group changes, a distance between the M1 lens group and the M2 lens group changes, and a distance between the M2 lens group and the RN lens group changes,

upon zooming, a lens group disposed closest to an image is moved,

upon focusing from an infinite distant object to a short distant object, the RN lens group moves, and

following conditional expressions are satisfied,

0.15<(−fTM1)/f1<0.35

0.264≤fTM2/f1<0.40

where

f1: a focal length of the front lens group,

fTM1: a focal length of the M1 lens group in a telephoto end state, and

fTM2: a focal length of the M2 lens group in a telephoto end state,

wherein the RN lens group comprises:

at least one lens having positive refractive power; and

at least one lens having negative refractive power.

2. The zoom optical system according to claim 1, wherein

the subsequent lens group comprises, in order from the object: a lens having a negative refractive power; and a lens having a positive refractive power.

3. The zoom optical system according to claim 2, wherein

a following conditional expression is satisfied,

0.70<(−fN)/fP<2.00

where

fN: a focal length of a lens having a strongest negative refractive power in the subsequent lens group, and

fP: a focal length of a lens having a strongest positive refractive power in the subsequent lens group.

4. The zoom optical system according to claim 1, wherein

upon zooming from a wide-angle end state to a telephoto end state, the front lens group moves toward the object.

5. The zoom optical system according to claim 1, wherein

the subsequent lens group comprises a negative meniscus lens that has a concave surface facing the object, and is adjacent to an image side of the RN lens group.

6. The zoom optical system according to claim 1, wherein

a following conditional expression is satisfied,

1.80<f1/fw<3.50

where

f1: a focal length of the front lens group, and

fw: a focal length of the zoom optical system in a wide-angle end state.

7. The zoom optical system according to claim 1, wherein

a following conditional expression is satisfied,

3.70<f1/(−fTM1)<5.00

where

f1: a focal length of the front lens group, and

fTM1: a focal length of the M1 lens group in a telephoto end state.

8. The zoom optical system according to claim 1, wherein

a following conditional expression is satisfied,

3.20<f1/fTM2<5.00

where

f1: a focal length of the front lens group, and

fTM2: a focal length of the M2 lens group in a telephoto end state.

9. The zoom optical system according to claim 1, wherein

upon zooming, a lens group nearest to the object in the M1 lens group is fixed with respect to an image surface.

10. The zoom optical system according to claim 1, wherein

the M2 lens group comprises a vibration-proof lens group movable in a direction orthogonal to an optical axis.

11. The zoom optical system according to claim 10, wherein

the vibration-proof lens group consists of, in order from the object: a lens having a negative refractive power;

and a lens having a positive refractive power.

12. The zoom optical system according to claim 11, wherein

a following conditional expression is satisfied,

1.00<nvrN/nvrP<1.25

where

nvrN: a refractive index of the lens having the negative refractive power in the vibration-proof lens group, and

nvrP: a refractive index of the lens having the positive refractive power in the vibration-proof lens group.

13. The zoom optical system according to claim 11, wherein

a following conditional expression is satisfied,

0.30<νvrN/νvrP<0.90

where

νvrN: an Abbe number of the lens having the negative refractive power in the vibration-proof lens group, and

νvrP: an Abbe number of the lens having the positive refractive power in the vibration-proof lens group.

14. The zoom optical system according to claim 1, wherein

the M1 lens group comprises a vibration-proof lens group movable in a direction orthogonal to an optical axis.

15. The zoom optical system according to claim 14, wherein

the vibration-proof lens group consists of, in order from the object: a lens having a negative refractive power; and a lens having a positive refractive power.

16. The zoom optical system according to claim 15, wherein

a following conditional expression is satisfied,

0.80<nvrN/nvrP<1.00

where

17. The zoom optical system according to claim 15, wherein

a following conditional expression is satisfied,

1.20<νvrN/νvrP<2.40

where

18. An optical apparatus comprising the zoom optical system according to claim 1.

19. An imaging apparatus comprising: the zoom optical system according to claim 1; and an imaging unit that takes an image formed by the zoom optical system.

20. A zoom optical system comprising, in order from an object: a front lens group having a positive refractive power; an M1 lens group having a negative refractive power; an M2 lens group having a positive refractive power; an RN lens group having a negative refractive power; and a subsequent lens group, wherein

upon zooming, a lens group disposed closest to an image is moved,

upon focusing from an infinite distant object to a short distant object, the RN lens group moves,

the subsequent lens group comprises a lens having a positive refractive power, and

following conditional expressions are satisfied,

0.20<fTM2/f1<0.40

1.80<f1/fw≤2.441

where

fTM2: a focal length of the M2 lens group in a telephoto end state,

f1: a focal length of the front lens group, and

fw: a focal length of the zoom optical system in a wide-angle end state.

21. The zoom optical system according to claim 20, wherein

a following conditional expression is satisfied,

0.15<(−fTM1)/f1<0.35

where

fTM1: a focal length of the M1 lens group in a telephoto end state.

22. The zoom optical system according to claim 20, wherein

a following conditional expression is satisfied,

3.70<f1/(−fTM1<5.00

where

fTM1: a focal length of the M1 lens group in a telephoto end state.

23. The zoom optical system according to claim 20, wherein

a following conditional expression is satisfied,

3.20<f1/fTM2<5.00.

24. An optical apparatus comprising the zoom optical system according to claim 20.

25. An imaging apparatus comprising: the zoom optical system according to claim 20; and an imaging unit that takes an image formed by the zoom optical system.

26. A method for manufacturing a zoom optical system comprising, in order from an object, a front lens group having a positive refractive power, an M1 lens group having a negative refractive power, an M2 lens group having a positive refractive power, an RN lens group having a negative refractive power, and a subsequent lens group,

the method comprising:

arranging the lens groups so that:

upon zooming, a lens group disposed closest to an image is moved, and

the method further comprising one of the following features A or B, wherein

the feature A comprises:

disposing each lens in a lens barrel so as to satisfy following conditional expressions:

0.15<(−fTM1)/f1<0.35

0.264≤fTM2/f1<0.40

where

f1: a focal length of the front lens group,

fTM1: a focal length of the M1 lens group in a telephoto end state, and

fTM2: a focal length of the M2 lens group in a telephoto end state, and

wherein the RN lens group comprises:

at least one lens having positive refractive power; and

at least one lens having negative refractive power, and

the feature B comprises:

arranging so that the subsequent lens group comprises a lens having a positive refractive power, and

0.20<fTM2/f1<0.40

1.80<f1/fw≤2.441

where

fTM2: a focal length of the M2 lens group in a telephoto end state,

f1: a focal length of the front lens group, and

fw: a focal length of the zoom optical system in a wide-angle end state.